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Strict forms of the nested mixing estimates — Remark 3.9
PDF p. 22: Remark 3.9
Statement
Let be an -expander as in Two-sided spectral expander — Definition 1.9, with and . Thus . For vertex subsets , let be the ordered adjacency count and as in Oriented edge count between sets. Let and put . If , , and , then the two bounds in Lemma 3.7 become strict:
If in addition , , , and , then the bound in Lemma 3.8 also becomes strict:
For a phase configuration and angles , these conclusions apply with and whenever these phase-tail sets are nested and satisfy the displayed hypotheses. Here for , as in Phase tail sets for amplification. The stronger size hypotheses , , and, for the second conclusion, are sufficient when the other stated conditions also hold.
Facts & Assumptions
The expander definition gives and , where order means nonnegative quadratic-form difference (Two-sided spectral expander — Definition 1.9).
For any subset , put . Its centered cut count lies between and (Cut-edge mixing bound — Lemma 3.4). For nested , twice equals the cut counts of and minus that of (Nested-cut polarization identity).
Internal-edge mixing gives (Internal-edge mixing bound — Lemma 3.3). Edge counts are nonnegative finite sums of adjacency entries (Oriented edge count between sets).
Lemmas 3.7 and 3.8 give the corresponding non-strict estimates under their stated hypotheses (Mixing for two nearby nested sets — Lemma 3.7, Relative mixing for a small nested set — Lemma 3.8).
Proof
Given: The expander, parameters and nested sets in the statement.
Goal: Establish the strict estimates and their phase-tail specialization.
Testing the difference of the order bounds in [F1] on a nonzero vector gives . Since and , and . Put , , and . The strict size condition says , so . Also , hence .
The three sets , , and partition . Thus , , , and . Applying [F2] to the three centered cuts, with the bound reversed for the subtracted cut, gives .
Because , , and , we have . Multiplication by and substitution into step 2.1 proves both strict bounds. These refine the non-strict bounds recorded in [F4].
For the additional hypotheses set . By [F3] and , . Step 3.1 and give . Since , the preceding internal-edge bound gives , proving the strict relative bound refining [F4].
The phase-tail definition identifies each displayed as a subset of . Substituting the two nested sets into steps 3.1 and 4.1 proves the specialization; each strict size hypothesis in the last sentence implies the corresponding weak hypothesis used above.
Source notes
Remark 3.9 of the cited article attributes the strictness observation. The estimates above are derived from the declared cut and internal-edge bounds. The conditions and, for the relative estimate, make the strictness argument explicit under the frozen expander definition; the article attribution alone is not used as proof.
Depends on
- Two-sided spectral expander — Definition 1.9
- Oriented edge count between sets
- Phase tail sets for amplification
- Nested-cut polarization identity
- Internal-edge mixing bound — Lemma 3.3
- Cut-edge mixing bound — Lemma 3.4
- Mixing for two nearby nested sets — Lemma 3.7
- Relative mixing for a small nested set — Lemma 3.8
Dependency tree · 2 levels
Each result is drawn at its shortest distance from this item. Arrows run from prerequisites to the items that use them; this item has a heavier outline. External source nodes link directly to the cited text. The view shows up to two dependency steps; open a prerequisite to continue.
Sources
- Expander graphs are globally synchronizing · PDF p. 22, Remark 3.9; pp. 24–26, amplification argument